In the review of Particle Data Group [1]}, all of the nucleon resonances with mass larger than 2150 MeV are listed as follows, \(N(2190)\) , \(N(2200)\) , \(N(2250)\) , \(N(2300)\) , \(N(2570)\) , \(N(2600)\)  and \(N(2700)\) .
Among these nucleon resonances, the \(N(2190)\) , \(N(2200)\) , \(N(2250)\) , \(N(2600)\) , and \(N(2700)\)  resonances are found from experiments based on \(\pi N,\gamma N\)  reactions [2]}, [3]}, [4]}, [5]}, [6]}, [7]}, while \(N(2300)\)  and \(N(2570)\)  are from the decay final states of \(\psi (2S)\)  [8]}.
In the analysis of \(\pi N\) , \(\gamma N\)  reactions, Bonn-Jülich group [9]} and ANL-Osaka group [10]} used dynamical coupled-channels approach to extract the \(N^*\)  resonances with various effective interactions.
Bonn-Gatchina group [11]} and GWU/SAID group [5]} used a K-matrix approach with Breit-Wigner resonances to analyze related channels.
And the KSU group [13]} used a generalized energy-dependent Breit-Wigner parametrization of amplitudes to treat these channels.
The spins of all these \(N^*\)  resonances with mass heavier than 2.15 GeV are found to be larger than 5/2.
However, from the \(\psi \)  decay, the two new \(N^*\)  resonances found by BES collaboration from partial wave analysis (PWA) of \(\psi ^{\prime } \rightarrow \bar{N} N^* + c.c. \rightarrow \bar{N}N\pi \)  have spin less than or equal to 5/2.
It is interesting to find that the spins of the heavy \(N^*\)  resonances generated from \(\pi N,\gamma N\)  reaction are obviously larger than these from the \(\psi \)  decay.
